Newton’s Second Law of Motion is often summarized as F = ma (force equals mass times acceleration). However, its more general form relates force to the rate of change of momentum:
\(F=\frac{dp}{dt}\)
Here, momentum (p) is the product of mass (m) and velocity (v): p = mv. This equation implies that force is directly tied to how quickly an object’s momentum changes over time.
When mass is constant, the law simplifies to F = ma, as acceleration (a) is the derivative of velocity. However, the momentum form ( \(F=\frac{dp}{dt}\)) is crucial for understanding scenarios involving varying mass or velocity, such as rocket motion or collisions.
Impulse (J) quantifies the total effect of a force acting over time. Mathematically, it’s the integral of force over a time interval (Δt):
\(J=\int_{t_1}^{t_2} F dt\)
From Newton’s Second Law, this integral equals the change in momentum (Δp):
J = Δp = pfinal − pinitial
For constant force, impulse simplifies to: J = Favg × Δt
An impulsive force acts over an extremely short duration (Δt → 0), producing a significant change in momentum. Examples include hammer strikes, car crashes, or a cricket bat hitting a ball. Using the impulse equation:
Favg = Δp / Δt
If Δt is tiny, Favg becomes very large even for modest momentum changes.
A cricket ball (m = 0.15 kg) accelerates from 0 to 20 m/s in 0.01 s:
Favg = (0.15 × 20) / 0.01 = 3 / 0.01 = 300 N
A 5 kg object experiences a force of 10 N for 3 s. Find its impulse and final velocity (if initial velocity is 2 m/s).
Impulse: J = F × Δt = 10 × 3 = 30 Ns
Δp = 30 = m(vf − vi)
⇒ vf = (30 / 5) + 2 = 8 m/s